Page 84 - Singiresu S. Rao-Mechanical Vibrations in SI Units, Global Edition-Pearson (2017)
P. 84

1.9  dampinG elements    81
                                    Equations (E.9) and (E.8) lead to

                                                                            2d
                                                                      3
                                                                  3pD l¢1 +   ≤
                                                                 C          D  S
                                                             P =                mv 0                   (E.10)
                                                                       4d 3
                                    By writing the force as P = cv 0 , the damping constant c can be found as
                                                                       3
                                                                    3pD l     2d
                                                              c = mJ     ¢1 +   ≤ R                    (E.11)
                                                                     4d 3     D
                                                                                                           ■



                 1.9.2              If the force (F)-velocity (v) relationship of a damper is nonlinear:
                 linearization                                                                         (1.26)
                 of a nonlinear                                     F = F1v2
                 damper             a linearization process can be used about the operating velocity 1v*2, as in the case of a
                                    nonlinear spring. The linearization process gives the equivalent damping constant as

                                                                       dF
                                                                   c =       2                         (1.27)
                                                                        dv  v*



                 1.9.3              In some dynamic systems, multiple dampers are used. In such cases, all the dampers are
                 Combination of     replaced by a single equivalent damper. When dampers appear in combination, we can
                 dampers            use procedures similar to those used in finding the equivalent spring constant of multiple
                                    springs to find a single equivalent damper. For example, when two translational dampers,
                                    with damping constants c  and c , appear in combination, the equivalent damping constant
                                                        1
                                                              2
                                    1c 2 can be found as (see Problem 1.55):
                                      eq
                                      Parallel dampers:  c eq  = c + c 2                               (1.28)
                                                           1
                                                      1    1    1
                                    Series dampers:     =    +                                         (1.29)
                                                     c eq  c 1  c 2



                                    equivalent spring and damping Constants of a machine tool support
                 example 1.17
                                    A precision milling machine is supported on four shock mounts, as shown in Fig. 1.45(a). The elas-
                                    ticity and damping of each shock mount can be modeled as a spring and a viscous damper, as shown
                                    in Fig. 1.45(b). Find the equivalent spring constant, k eq , and the equivalent damping constant, c eq ,
                                    of the machine tool support in terms of the spring constants 1k i 2 and damping constants 1c i 2 of
                                    the mounts.
   79   80   81   82   83   84   85   86   87   88   89